Conceptual

QFT2 Lecture 2a: Intro to interacting theories

The core principle established is that interacting Quantum Field Theories (QFT) cannot be solved exactly and must instead be treated via perturbation theory relative to a free field solution, parameterized by the coupling constant Lambda. This approach relies on decomposing correlation functions into spectral densities defined over physical states; specifically, rho(m^2), which encodes the probability of creating multi-particle or bound states versus single-particle poles characterized by the wavefunction renormalization constant Z. The theoretical significance lies in mapping how interactions modify vacuum-to-state amplitudes, determining particle stability and scattering probabilities while maintaining consistency with the parent discipline's framework of relativistic quantum mechanics.